What is the form of momentum which is conserved in electrodynamics? It isn't mv+qA the canonical momentum. Is it mv-qA as mentioned in my2cts answer[here](https://physics.stackexchange.com/questions/114466)
I doubt because the field contribution(volume integral of Poynting vector) isn't being accounted there..
there's also a founding effect where many of the initial members were hep-th theorists and so the site was seeded with such questions being overrepresented
I left an open beer in the freezer while monitoring its temperature. The first minutes works as expected. But after the plateau, at about −8 °C, a peak appeared:
I thought it was an artefact because the can was open and the sensor was inside.
So I repeated the experiment with an intact, closed c...
There's no argument given for the gravitational field vanishing at infinity, it's just stated as an assumption. It doesn't seem to be used anywhere else in L&L and it's not even really used except for being framed as an essential difference between a non-inertial frame and a gravitational field, there's something subtle here at least
The comment is actually in the section on non-relativistic gravitational fields and not in the relativistic section, they don't give this argument in the relativistic section, maybe I am wrong thinking it also applies there, but even in the non-relativistic section, why is this an okay assumption if your model is just $L = mv^2/2 - m \phi$,
We can concoct solutions which don't go to zero at infinity right
It's Poisson with complicated boundary conditions at infinity, can you have solutions or are they impossible
If not then that is probably what's going on with the quote, if you can then maybe it's a physical assumption to exclude them because we are biased by Newton
This question does not seem to have a single correct answer posted.
Which of the following are true:
Assume that there will never be one right answer posted (i.e. because there is not in principle a right answer).
This was a bad question and should be closed/deleted.
Leave it how it is. It's ok...
It's one of those issues physicists don't really care about anymore
it was of some concern in the 19th century but then GR happened a bit later so people kind of stopped caring
A few philosophers of physics talk about it and I don't remember if the conclusion is that it's "physical" or not
the rough idea being that if there's uniform matter distribution (so non-zero potential at infinity), then things diverge, and no matter what regularizing procedure you try to use, it will still not make sense in some way
Poisson's equation is an elliptic partial differential equation of broad utility in theoretical physics. For example, the solution to Poisson's equation is the potential field caused by a given electric charge or mass density distribution; with the potential field known, one can then calculate electrostatic or gravitational (force) field. It is a generalization of Laplace's equation, which is also frequently seen in physics. The equation is named after French mathematician and physicist Siméon Denis Poisson.
== Statement of the equation ==
Poisson's equation is
Δ...
(I think) There's a boundary term missing in the Green function solution they give, maybe even in Newtonian GR this is just an assumption and one can ask why we can't assume it in GR too